NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = J.P.Connelly Found 19 matches. 1998CO06 Phys.Rev. C57, 1569 (1998) J.P.Connelly, B.L.Berman, W.J.Briscoe, K.S.Dhuga, A.Mokhtari, D.Zubanov, H.P.Blok, R.Ent, J.H.Mitchell, L.Lapikas Trinucleon Cluster Knockout from 6Li NUCLEAR REACTIONS 6Li(e, e'3He), E=484.5 MeV; 6Li(e, e't), E=456, 524 MeV; measured σ(E, θ) momentum transfer dependence; deduced two-step processes.
doi: 10.1103/PhysRevC.57.1569
1995PE01 Phys.Rev. C51, 1014 (1995) M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, S.Raman Low-Multipolarity Magnetic Transitions in 40Ca Excited by 180° Electron Scattering NUCLEAR REACTIONS Ca, S(e, e'), E=28.4-56.5 MeV; measured σ(θ); deduced σ. 40Ca levels deduced B(λ). Model comparison.
doi: 10.1103/PhysRevC.51.1014
1994PE08 Phys.Rev. C49, 3000 (1994) M.Petraitis, J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, D.I.Sober, J.R.Deininger, S.E.Williamson, R.Lindgren, S.Raman Low-Multipolarity Magnetic Transitions in 30Si, 32S, and 34S Studied by 180° Electron Scattering NUCLEAR REACTIONS 30Si, 32,34S(e, e'), E=28.4-63.4 MeV; measured spectra, σ. 32,34S, 30Si deduced M1, M2 transition strength fragmentation features.
doi: 10.1103/PhysRevC.49.3000
1993KE03 Phys.Rev. C47, 2146 (1993) J.J.Kelly, B.S.Flanders, F.W.Hersman, J.H.Heisenberg, J.Calarco, J.P.Connelly, T.E.Milliman, A.Scott, F.T.Baker, V.Penumetcha, W.P.Jones, G.T.Emery, A.D.Bacher, C.Olmer, M.A.Grimm, M.L.Whiten Neutron Transition Densities from 88Sr(p, p') at E(p) = 200 MeV NUCLEAR REACTIONS 88Sr(polarized p, p'), (polarized p, p), E=200 MeV; measured σ(θ), analyzing power vs θ. 88Sr levels deduced neutron transition densities. Shell model comparison.
doi: 10.1103/PhysRevC.47.2146
1993WI08 Phys.Rev. C47, 2539 (1993) J.E.Wise, J.R.Calarco, J.P.Connelly, S.A.Fayans, F.W.Hersman, J.H.Heisenberg, R.S.Hicks, W.Kim, T.E.Milliman, R.A.Miskimen, G.A.Peterson, A.P.Platonov, E.E.Saperstein, R.P.Singhal Ground-State Magnetization Density of 89Y NUCLEAR REACTIONS 89Y(e, e), E=71-262 MeV; measured σ(θ), θ=180°. 89Y deduced ground state M1 form factor. Fourier-Bessel analysis.
doi: 10.1103/PhysRevC.47.2539
1992CO03 Phys.Lett. 277B, 383 (1992) J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, S.Raman, J.R.Deininger, S.E.Williamson Magnetic Dipole Strength in 46Ca Observed with 180° Electron Scattering NUCLEAR REACTIONS 46Ca(e, e'), E=32.9-63.1 MeV; measured σ(E(e')), θ=180°; deduced σ(θ). 46Ca level deduced reduced transition rate, transition radius, B(λ).
doi: 10.1016/0370-2693(92)91798-E
1992CO07 Phys.Rev. C45, 2494 (1992) J.P.Connelly, H.Crannell, L.W.Fagg, J.T.O'Brien, M.Petraitis, D.I.Sober, J.R.Deininger, S.E.Williamson Low-Momentum-Tranfer 180° Electron Scattering from the 3.68 MeV (3/2)- and the 3.85 MeV (5/2)+ States in 13C NUCLEAR REACTIONS 13C(e, e'), E=28.5-56.5 MeV; measured σ(E(e')), σ(θ), transverse form factors. 13C levels deduced B(λ).
doi: 10.1103/PhysRevC.45.2494
1992CO14 Phys.Rev. C45, 2711 (1992) J.P.Connelly, D.J.DeAngelis, J.H.Heisenberg, F.W.Hersman, W.Kim, M.Leuschner, T.E.Milliman, J.Wise, C.N.Papanicolas High Resolution Electron Scattering from High Spin States in 208Pb NUCLEAR REACTIONS 208Pb(e, e'), E=100-300 MeV; measured σ(E(e')), form factors. 208Pb deduced high spin states quenching, 12- state transition strength fragmentation. Independent particle model, DWBA.
doi: 10.1103/PhysRevC.45.2711
1992KI10 Phys.Rev. C45, 2290 (1992) W.Kim, B.L.Miller, J.R.Calarco, L.S.Cardman, J.P.Connelly, S.A.Fayans, B.Frois, D.Goutte, J.H.Heisenberg, F.W.Hersman, V.Meot, T.E.Milliman, P.Mueller, C.N.Papanicolas, A.P.Platonov, V.Yu.Ponomarev, J.E.Wise Interplay between Single-Particle and Collective Degrees of Freedom in the Excitation of the Low-Lying States in 140Ce NUCLEAR REACTIONS 140Ce(e, e'), E=190 MeV; measured σ(E(e')), θ=45°. 140Ce levels deduced form factors, transition charge densities, B(λ), configurations. Quasiparticle-phonon model, self-consistent finite Fermi system theory.
doi: 10.1103/PhysRevC.45.2290
1992KI20 Phys.Rev. C46, 1656 (1992) W.Kim, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.Wise, C.N.Papanicolas, S.A.Fayans, A.P.Platonov Ground-State Charge Distribution and Transition Charge Densities of the Low-Lying States in 86Sr NUCLEAR REACTIONS 86Sr(e, e'), (e, e), E=100-370 MeV; measured form factors. 86Sr levels deduced B(λ), transition charge densities.
doi: 10.1103/PhysRevC.46.1656
1992OB01 Nucl.Instrum.Methods Phys.Res. A312, 531 (1992) J.T.O'Brien, D.I.Sober, L.W.Fagg, H.Crannell, M.Petraitis, J.P.Connelly, J.R.Deininger, S.E.Williamson Design and Testing of Apparatus for 180° Electron Scattering at Low Momentum-Transfer NUCLEAR REACTIONS 28Si, 13C(e, e), E=53 MeV; measured electron spectra, before, after focal plane corrections. Low momentum transfer, 180° electron scattering appartus design and testing.
doi: 10.1016/0168-9002(92)90201-E
1992WI06 Phys.Rev. C45, 2701 (1992) J.E.Wise, J.P.Connelly, F.W.Hersman, J.H.Heisenberg, W.Kim, M.Leuschner, S.A.Fayans, A.P.Platonov, E.E.Saperstein, V.Yu.Ponomarev Transition Densities of Collective Excitations in 118Sn NUCLEAR REACTIONS 118Sn(e, e), (e, e'), E=252, 376 MeV; measured σ(θ, E(e')). 118Sn levels deduced transition charge densities, B(λ). Finite Fermi system, quasiparticle-phonon approach.
doi: 10.1103/PhysRevC.45.2701
1991KI13 Phys.Rev. C44, 2400 (1991) W.Kim, J.R.Calarco, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, T.E.Milliman, J.E.WIse, B.L.Miller, C.N.Papanicolas, V.Yu.Ponomarev, E.E.Saperstein, A.P.Platonov Properties of Low-Lying States in 142Ce via High Resolution Electron Scattering NUCLEAR REACTIONS 142Ce(e, e'), E=100-370 MeV; measured reaction products, Eβ, Iβ; deduced σ(E(e'), θ=45°), form factors, B(E2). 142Ce levels deduced charge densities. Quasiparticle-phonon approach, finite Fermi system.
doi: 10.1103/PhysRevC.44.2400
1990CO25 Phys.Rev. C42, 1948 (1990) J.P.Connelly, T.E.Milliman, J.H.Heisenberg, F.W.Hersman, J.E.Wise, C.N.Papanicolas Proton Core Polarization in Low-Lying States of 86Sr NUCLEAR REACTIONS 92Mo(e, e'), E=200 MeV; 86Sr(e, e'), E=190 MeV; measured σ(θ). 92Mo, 86Sr levels deduced transition charge densities.
doi: 10.1103/PhysRevC.42.1948
1990HA09 Phys.Rev. C41, 1619 (1990) K.Hansen, J.-O.Adler, K.I.Blomqvist, D.Nilsson, A.Sandell, B.Schroder, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, J.R.Calarco, J.P.Connelly, F.W.Hersman, W.Kim, M.Leuschner Electrofission in the Quasifree and Delta Regions NUCLEAR REACTIONS 233,238U(e, e'F), E=720-830 MeV; measured σ(E, θ), fission probability; deduced mean nuclear excitation energy. Parallel plate avalanche detector.
doi: 10.1103/PhysRevC.41.1619
1990MI07 Phys.Rev. C41, 2586 (1990) T.E.Milliman, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, J.E.Wise, C.N.Papanicolas Electron Scattering from 92Mo NUCLEAR REACTIONS 92Mo(e, e'), E=189.6 MeV; measured σ(θ), σ(E(e')). 92Mo levels deduced J, π, transition charge, current densities. Other data analyzed.
doi: 10.1103/PhysRevC.41.2586
1990WI13 Phys.Rev. C42, 1077 (1990) J.E.Wise, F.W.Hersman, J.H.Heisenberg, T.E.Milliman, J.P.Connelly, J.R.Calarco, C.N.Papanicolas Single-Particle Excitations in 89Y NUCLEAR REACTIONS 89Y(e, e'), E=370.9, 622.8 MeV; measured σ(θ), form factors. 89Y deduced transition charge, current densities. DWBA analysis, shell model. NUCLEAR STRUCTURE 89Y; calculated levels, transition charge, current densities. Shell model.
doi: 10.1103/PhysRevC.42.1077
1988MI05 Phys.Rev. C37, 895 (1988) B.L.Miller, L.S.Cardman, C.N.Papanicolas, T.E.Milliman, J.P.Connelly, J.H.Heisenberg, F.W.Hersman, J.E.Wise, B.Frois, D.Goutte, V.Meot Electroexcitation of High-Multipolarity Transitions in 140Ce NUCLEAR REACTIONS 140Ce(e, e'), E=100-370 MeV; measured σ(E(e')), σ(θ). 140Ce deduced level, J, π, configuration, γ-multipolarity, quenching factor.
doi: 10.1103/PhysRevC.37.895
1985MI15 Phys.Rev. C32, 805 (1985) T.E.Milliman, J.H.Heisenberg, F.W.Hersman, J.P.Connelly, C.N.Papanicolas, J.E.Wise, H.P.Blok, L.T.van der Bijl Determination of the π1g9/2 Orbit Size in 88Sr, 90Zr, and 92Mo from Inelastic Electron Scattering NUCLEAR STRUCTURE 88Sr, 90Zr, 92Mo; calculated spectroscopic amplitudes for 8+ transitions, rms radii of 1g9/2 proton orbit. Shell model, electron scattering data input. NUCLEAR REACTIONS 88Sr, 90Zr, 92Mo(e, e'), E=100-370 MeV; measured σ(E, θ) vs momentum transfer for 8+ states. 88Sr, 90Zr, 92Mo deduced point proton density. Shell model.
doi: 10.1103/PhysRevC.32.805
Back to query form |